相关实验视频
Updated: Jun 6, 2025

07:36
Fabricating Nanogaps by Nanoskiving
Published on: May 13, 2013
11.1K
探讨 - - 烯晶体中的宽半导体特性:密度函数理论的见解
T A Santos1, R B Marques2, A M Silva3
1PPGQ-GERATEC, State University of Piauí, 64002-150, Teresina, PI, Brazil.
Journal of molecular modeling
|November 30, 2024
概括
这项研究探讨了 (1S) -α-pinene晶体的纳米电子潜力. 理论计算显示了宽带间隙,将其归类为适用于先进电子应用的半导体.
科学领域:
- 固态物理 固态物理
- 计算化学的计算化学
- 材料科学 材料科学 材料科学
背景情况:
- 来自针叶树的天然单烯α-pinene具有药理潜力.
- 它的晶体结构和电子特性是理解其应用的关键.
- 宽带间隙材料对于下一代纳米电子技术至关重要.
研究的目的:
- 从理论上研究 (1S) - 烯晶体的结构和电子特性.
- 根据其带隙,评估其用于纳米电子应用的潜力.
- 分析电子结构并确定化学相互作用的潜在地点.
主要方法:
- 密度函数理论 (DFT) 计算使用量子埃斯普雷索.
- 采用了局部密度近似方法 (LDA-PZ) 和通用梯度近似方法 (GGA-PBE).
- 为了准确的核心电子表示,利用了保持规范的伪电位.
主要成果:
- 每个单元细胞有104个原子的正方形晶体结构,与实验数据相匹配.
- 计算的间接频段间隙为3.58 eV (LDA-PZ) 和4.32 eV (GGA-PBE). 这些间接频段间隙为3.58 eV (LDA-PZ).
- 确定了C和H原子轨道作为电子结构的主要贡献者.
结论:
- (1S) -α-pinene晶体表现出宽带间隙半导体特性.
- 该材料在纳米电子设备应用中显示出前景.
- 电子结构分析表明有针对性的化学修饰的潜力.
相关概念视频
Types of Semiconductors
534
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
534
Fermi Level Dynamics
225
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
225
Band Theory
15.0K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
15.0K
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds
1.2K
In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
1.2K
¹H NMR: Long-Range Coupling
1.7K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
1.7K

